Bootstrapping the chiral-gravitational anomaly

A bstract We analyze causality and unitarity constraints in graviton scattering amplitudes, aiming to establish new bounds on theories with U(1)-gravitational anomalies, such as axion models or strongly-coupled gauge theories. For this purpose, we show the necessity of coupling these theories to gravity. We obtain a universal scale Λ caus at which states with J ≥ 4 must appear in the theory. We show that this scale can lie below the quantum gravity scale. For axion models, we get Λ caus ∼ $$\sqrt{{M}_{P}{f}_{a}}$$ where f a is the axion decay constant. In strongly-coupled gauge theories in the large- N c limit, the presence of glueballs allows to evade these bounds, provided the number of fermions N F ≪ N c and the ’tHooft coupling is not large. Nevertheless, for models that have a holographic 5D dual (large ’tHooft coupling), Λ caus emerges as a new cutoff scale, unless certain conditions on the parameters of the 5D models are satisfied.

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-05-14
DOI
https://doi.org/10.1007/jhep05(2025)114
Citations
6
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
11.22

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article

Bootstrapping the chiral-gravitational anomaly

Zi-Yu Dong, Francesco Sciotti, Alex Pomarol, T. Ma
6 citations
Journal of High Energy Physics
Black Holes and Theoretical Physics
11.22
article

Bootstrapping the chiral-gravitational anomaly

Zi-Yu Dong, Francesco Sciotti, Alex Pomarol, T. Ma
article en
6 citations

Abstract

A bstract We analyze causality and unitarity constraints in graviton scattering amplitudes, aiming to establish new bounds on theories with U(1)-gravitational anomalies, such as axion models or strongly-coupled gauge theories. For this purpose, we show the necessity of coupling these theories to gravity. We obtain a universal scale Λ caus at which states with J ≥ 4 must appear in the theory. We show that this scale can lie below the quantum gravity scale. For axion models, we get Λ caus ∼ $$\sqrt{{M}_{P}{f}_{a}}$$ where f a is the axion decay constant. In strongly-coupled gauge theories in the large- N c limit, the presence of glueballs allows to evade these bounds, provided the number of fermions N F ≪ N c and the ’tHooft coupling is not large. Nevertheless, for models that have a holographic 5D dual (large ’tHooft coupling), Λ caus emerges as a new cutoff scale, unless certain conditions on the parameters of the 5D models are satisfied.

Journal of High Energy PhysicsVol. 2025(5)
Universitat Autònoma de Barcelona (ES), University of Chinese Academy of Sciences (CN)
Chinese Academy of Sciences, Agencia Estatal de Investigación
Openalex Percentile: Top 2%
Black Holes and Theoretical Physics
11.22
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